[go: up one dir, main page]

US3943884A - Fluidic frequency generator - Google Patents

Fluidic frequency generator Download PDF

Info

Publication number
US3943884A
US3943884A US05/435,362 US43536274A US3943884A US 3943884 A US3943884 A US 3943884A US 43536274 A US43536274 A US 43536274A US 3943884 A US3943884 A US 3943884A
Authority
US
United States
Prior art keywords
helix
gas
sleeve
sub
generator according
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US05/435,362
Inventor
Charles Peter Majkrzak
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
ITT Inc
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Priority to US05/435,362 priority Critical patent/US3943884A/en
Application granted granted Critical
Publication of US3943884A publication Critical patent/US3943884A/en
Assigned to ITT CORPORATION reassignment ITT CORPORATION CHANGE OF NAME (SEE DOCUMENT FOR DETAILS). Assignors: INTERNATIONAL TELEPHONE AND TELEGRAPH CORPORATION
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/05Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects
    • G01F1/20Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects by detection of dynamic effects of the flow
    • G01F1/32Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects by detection of dynamic effects of the flow using swirl flowmeters
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/66Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by measuring frequency, phase shift or propagation time of electromagnetic or other waves, e.g. using ultrasonic flowmeters
    • G01F1/666Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by measuring frequency, phase shift or propagation time of electromagnetic or other waves, e.g. using ultrasonic flowmeters by detecting noise and sounds generated by the flowing fluid

Definitions

  • This invention relates to a fluidic frequency generator and more particularly to a fluidic frequency generator whose output frequency in cycles per second (cps) is proportional to the pressure in terms of pounds per square inch (psi) of a gas applied to the input thereof or to the changes in the mass rate of gas flow through the generator.
  • the object of the present invention is to provide a fluidic frequency generator whose output frequency is proportional to either of the above mentioned predetermined characteristics of gas flowing through the fluidic frequency generator.
  • a feature of the present invention is the provision of a fluidic frequency generator comprising: a helix of wire having predetermined dimensions; and a sleeve of selected material disposed to encircle and conform to the exterior surface configuration of the helix; the helix and the sleeve cooperating to provide at one end thereof an audio frequency in response to a gas applied to the other end thereof, the audio frequency being proportional to a predetermined characteristic of the gas flowing through the helix and the sleeve.
  • FIG. 1 is an elevational view partially in cross-section of a first embodiment of a fluidic frequency generator in accordance with the principles of the present invention
  • FIG. 2 is a cross-sectional view taken along line 2--2 of FIG. 1;
  • FIG. 3 is a testing arrangement to enable determining the relationship between a predetermined characteristic of a gas applied to the input of and the frequency of the audio frequency signal output of the fluidic frequency generator of FIG. 1;
  • FIG. 4 is a longitudinal cross-sectional view of a second embodiment of a fluidic frequency generator in accordance with the principles of the present invention.
  • FIGS. 1 and 2 there is illustrated therein a first embodiment of a fluidic frequency generator in accordance with the principles of the present invention which includes a helix 1 of wire, such as music wire and a sleeve 2 of a selected material, such as plastic, encircling helix 1 and conforming to the exterior surface configuration of helix 1.
  • a helix 1 of wire such as music wire
  • a sleeve 2 of a selected material such as plastic
  • the length of the resulting tube is 10 inches long
  • the helix 1 is formed of music wire having a diameter of 0.075 inches and a pitch diameter of 0.370 inches with six turns per inch while the plastic sleeve 2 has a thickness of 0.010 inches and is shrunk over helix 1.
  • the outer diameter of the combined helix and plastic sleeve has a dimension of 0.437 inches.
  • the fluidic frequency generator of FIG. 1 will have utility as a gas pressure to frequency translator, a mass rate of gas flow to frequency translator, a gas logic circuit component and a monitoring device for the mass rate of gas flow in a tube.
  • FIG. 4 there is illustrated therein a second embodiment of a fluidic frequency generator in accordance with the principles of the present invention which includes a helix 1a of wire, such as music wire and a sleeve 2a of metal encircling helix 1a.
  • a helix 1a of wire such as music wire
  • a sleeve 2a of metal encircling helix 1a The operation of this embodiment is as described with respect to the first embodiment of FIGS. 1 and 2.

Landscapes

  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Electrostatic, Electromagnetic, Magneto- Strictive, And Variable-Resistance Transducers (AREA)

Abstract

A helix of wire having predetermined dimensions is encircled by a sleeve of selected material which conforms to the exterior surface configuration of the helix. When a gas is applied into one end of the helix-sleeve combination, an audio frequency signal appears at the other end of the helix-sleeve combination having a frequency which increases in steps proportional to the entrance pressure of the gas flowing through the helix-sleeve combination, or proportional the changes in the mass rate of flow of the gas through the helix-sleeve combination.

Description

BACKGROUND OF THE INVENTION
This invention relates to a fluidic frequency generator and more particularly to a fluidic frequency generator whose output frequency in cycles per second (cps) is proportional to the pressure in terms of pounds per square inch (psi) of a gas applied to the input thereof or to the changes in the mass rate of gas flow through the generator.
SUMMARY OF THE INVENTION
The object of the present invention is to provide a fluidic frequency generator whose output frequency is proportional to either of the above mentioned predetermined characteristics of gas flowing through the fluidic frequency generator.
A feature of the present invention is the provision of a fluidic frequency generator comprising: a helix of wire having predetermined dimensions; and a sleeve of selected material disposed to encircle and conform to the exterior surface configuration of the helix; the helix and the sleeve cooperating to provide at one end thereof an audio frequency in response to a gas applied to the other end thereof, the audio frequency being proportional to a predetermined characteristic of the gas flowing through the helix and the sleeve.
BRIEF DESCRIPTION OF THE DRAWING
Above-mentioned and other features and objects of this invention will become more apparent by reference to the following description taken in conjunction with the accompanying drawing, in which:
FIG. 1 is an elevational view partially in cross-section of a first embodiment of a fluidic frequency generator in accordance with the principles of the present invention;
FIG. 2 is a cross-sectional view taken along line 2--2 of FIG. 1;
FIG. 3 is a testing arrangement to enable determining the relationship between a predetermined characteristic of a gas applied to the input of and the frequency of the audio frequency signal output of the fluidic frequency generator of FIG. 1; and
FIG. 4 is a longitudinal cross-sectional view of a second embodiment of a fluidic frequency generator in accordance with the principles of the present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Referring to FIGS. 1 and 2, there is illustrated therein a first embodiment of a fluidic frequency generator in accordance with the principles of the present invention which includes a helix 1 of wire, such as music wire and a sleeve 2 of a selected material, such as plastic, encircling helix 1 and conforming to the exterior surface configuration of helix 1.
In a reduction to practice of fluidic frequency generator of FIG. 1 the length of the resulting tube is 10 inches long, the helix 1 is formed of music wire having a diameter of 0.075 inches and a pitch diameter of 0.370 inches with six turns per inch while the plastic sleeve 2 has a thickness of 0.010 inches and is shrunk over helix 1. The outer diameter of the combined helix and plastic sleeve has a dimension of 0.437 inches.
When the fluidic frequency generator was tested employing the arrangement of FIG. 3, the relationship between the output frequency with increasing input gas or air pressure was observed and are presented hereinbelow in Table I. The frequencies produced as indicated in Table I were observed on the frequency meter 3, such as an oscilloscope, to be fairly pure and occurred in stepped transitions as illustrated in Table I.
              TABLE I                                                     
______________________________________                                    
           OUTPUT                                                         
PRESSURE   FREQUENCY     MULTIPLYING                                      
in psi     in cps        FACTOR                                           
______________________________________                                    
           1250          1                                                
           1680                                                           
           2500          2                                                
           2850                                                           
           3570                                                           
20         5000          4                                                
______________________________________                                    
The reason that the fluidic frequency generator of FIG. 1 produces the frequencies illustrated in Table I with increasing pressure of the input gas is believed to be due to the fact that a gas or air column vibrates sympathetically to set up stationary waves that have a frequency proportional to the pressure of the input gas.
Employing the fluidic frequency generator of FIG. 1 having the dimensions as set forth hereinabove wherein the length (L) is 10 inches or 0.835 feet the theory of vibration of air columns as applied to open tubes is applied to the fluidic frequency generator of FIG. 1 and the following information was obtained as indicated in Table II.
              TABLE II                                                    
______________________________________                                    
Fundamental Wavelength:                                                   
                λ = 2/1 L = 1.67  ft. at f.sub.f                   
First Overtone  λ = 2/2 L =  .835 ft. at f.sub.1                   
Second Overtone λ = 2/3 L =  .566 ft. at f.sub.2                   
Third Overtone  λ = 2/4 L =  .417 ft. at f.sub.3                   
Fourth Overtone λ = 2/5 L =  .334 ft. at f.sub.4                   
Fifth Overtone  λ = 2/6 L =  .278 ft. at f.sub.5                   
Sixth Overtone  λ = 2/7 L =  .239 ft. at f.sub.6                   
Seventh Overtone                                                          
                λ = 2/8 L =  .209 ft. at f.sub.7                   
______________________________________                                    
Accordingly, based upon f = c/λ, where c is equal to the velocity of sound at room temperature and atmospheric pressure and is equal to 1090 ft./sec., there is obtained as shown in Table III the frequencies of vibration of each of the wavelengths presented in Table II.
              TABLE III                                                   
______________________________________                                    
f.sub.f = 1090/1.67 =  652 cps                                            
                 f.sub.4 = 1090/.334 = 3260 cps                           
f.sub.1 = 1090/.835 = 1305 cps                                            
                 f.sub.5 = 1090/.278 = 3920 cps                           
f.sub.2 = 1090/.566 = 1930 cps                                            
                 f.sub.6 = 1090/.239 = 4560 cps                           
f.sub.3 = 1090/.417 = 2610 cps                                            
                 f.sub.7 = 1090/.209 = 5200 cps                           
______________________________________                                    
It has been determined experimentally that the frequencies in Table III are not quite correct since radiation from the open end of the open tube has been neglected. To take account of this, the length L in the formula of Table II must be slightly increased. If, for instance, a 5% correction were applied, the truer frequency for the open tube of 10 inches in length would be as shown below in Table IV.
              TABLE IV                                                    
______________________________________                                    
           ACTUAL                                                         
           MEASURED                                                       
THEORETICAL                                                               
           VALUES                                                         
VALUES     OF GEN.                                                        
FOR OPEN TUBE                                                             
           OF FIG. 1     VARIATION                                        
______________________________________                                    
f.sub.f =  620                                                            
f.sub.1 = 1245                                                            
           f.sub.1 = 1250                                                 
                         <1%                                              
f.sub.2 = 1830                                                            
           f.sub.2 = 1680                                                 
                          9%                                              
f.sub.3 = 2480                                                            
           f.sub.3 = 2500                                                 
                         <1%                                              
f.sub.4 = 3100                                                            
           f.sub.4 = 2850                                                 
                          9%                                              
f.sub.5 = 3730                                                            
           f.sub.5 = 3750                                                 
                         <1%                                              
f.sub.6 = 4350                                                            
           f.sub.6 =  ?  ?                                                
f.sub.7 = 4950                                                            
           f.sub.7 = 5000                                                 
                         <1%                                              
______________________________________                                    
As can be seen from the above open tube analysis as found in Tables II-IV, there is a close correlation between the excitation of the open tube and that of the fluidic frequency generator of FIG. 1. It should be noted that a particular vibrating frequency is triggered and maintained by a particular mass rate of gas flow through the configuration disclosed in FIG. 1. Thus, it is possible to use the configuration of the fluidic frequency generator of FIG. 1 to monitor changes in the mass rate of gas flow through a tube.
The fluidic frequency generator of FIG. 1 will have utility as a gas pressure to frequency translator, a mass rate of gas flow to frequency translator, a gas logic circuit component and a monitoring device for the mass rate of gas flow in a tube.
Referring to FIG. 4, there is illustrated therein a second embodiment of a fluidic frequency generator in accordance with the principles of the present invention which includes a helix 1a of wire, such as music wire and a sleeve 2a of metal encircling helix 1a. The operation of this embodiment is as described with respect to the first embodiment of FIGS. 1 and 2.
While I have described above the principles of my invention in connection with specific apparatus it is to be clearly understood that this description is made only by way of example and not as a limitation to the scope of my invention as set forth in the objects thereof and in the accompanying claims.

Claims (9)

I claim:
1. A fluidic frequency generator comprising:
a helix of wire having predetermined dimensions;
a sleeve of selected material disposed to encircle and conform to the exterior surface configuration of said helix; and
means containing a pressurized gas having a pressure greater than the atmosphere, said means being coupled to one end of said helix and said sleeve to direct said pressurized gas for flow through said helix and said sleeve from said one end to the other end of said helix and said sleeve;
said helix and said sleeve cooperating to provide at said other end an audio frequency in response to said gas flowing through said helix and said sleeve, said audio frequency being proportional to a predetermined characteristic of said gas flowing through said helix and said sleeve.
2. A generator according to claim 1, wherein
said predetermined characteristic is the pressure of said gas.
3. A generator according to claim 1, wherein
said predetermined characteristic is the change in the mass rate of flow of said gas.
4. A generator according to claim 1, wherein
said selected material is a plastic material.
5. A generator according to claim 4, wherein
said predetermined characteristic is the pressure of said gas.
6. A generator according to claim 4, wherein
said predetermined characteristic is the change in the mass rate of flow of said gas.
7. A generator according to claim 1, wherein
said selected material is a metal.
8. A generator according to claim 7, wherein
said predetermined characteristic is the pressure of said gas.
9. A generator according to claim 7, wherein
said predetermined characteristic is the change in the mass rate of flow of said gas.
US05/435,362 1974-01-21 1974-01-21 Fluidic frequency generator Expired - Lifetime US3943884A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US05/435,362 US3943884A (en) 1974-01-21 1974-01-21 Fluidic frequency generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US05/435,362 US3943884A (en) 1974-01-21 1974-01-21 Fluidic frequency generator

Publications (1)

Publication Number Publication Date
US3943884A true US3943884A (en) 1976-03-16

Family

ID=23728086

Family Applications (1)

Application Number Title Priority Date Filing Date
US05/435,362 Expired - Lifetime US3943884A (en) 1974-01-21 1974-01-21 Fluidic frequency generator

Country Status (1)

Country Link
US (1) US3943884A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3130722A1 (en) * 1980-08-16 1982-04-08 The Victoria University Of Manchester, Manchester FLUID FLOW MEASURING DEVICE
US4461651A (en) * 1983-02-08 1984-07-24 Foster Wheeler Limited Sonic cleaning device and method
CN110292828A (en) * 2019-07-31 2019-10-01 中国计量大学 A kind of water lift disappears white device and its water lift disappears whitening method

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2720221A (en) * 1952-12-23 1955-10-11 Electro Hydraulics Ltd Flexible metallic hose
US2986169A (en) * 1957-03-18 1961-05-30 Lee Rubber & Tire Corp Flexible hose

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2720221A (en) * 1952-12-23 1955-10-11 Electro Hydraulics Ltd Flexible metallic hose
US2986169A (en) * 1957-03-18 1961-05-30 Lee Rubber & Tire Corp Flexible hose

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3130722A1 (en) * 1980-08-16 1982-04-08 The Victoria University Of Manchester, Manchester FLUID FLOW MEASURING DEVICE
US4393721A (en) * 1980-08-16 1983-07-19 The Victoria University Of Manchester Apparatus for measuring fluid flow
US4461651A (en) * 1983-02-08 1984-07-24 Foster Wheeler Limited Sonic cleaning device and method
CN110292828A (en) * 2019-07-31 2019-10-01 中国计量大学 A kind of water lift disappears white device and its water lift disappears whitening method
CN110292828B (en) * 2019-07-31 2023-06-23 中国计量大学 Water extraction and whitening device and water extraction and whitening method thereof

Similar Documents

Publication Publication Date Title
US3648512A (en) Methods and apparatus for measuring the densities of fluids
Ort et al. Influence of mountiing on the accuracy of piezoelectric pressure measurements for hypersonic boundary layer transition
US2365015A (en) Fluid pressure gauge
US4201092A (en) Method of detecting and monitoring a leak caused by a through wall crack in a high pressure fluid system
US2362589A (en) Dynamometer and extensometer for impact testing
US2837914A (en) Acoustic impedance measuring apparatus
CN109765181B (en) Differential type resonance photoacoustic cell for improving gas photoacoustic spectrum detection stability
US3943884A (en) Fluidic frequency generator
US2568277A (en) Fluid testing apparatus
US2604787A (en) Acoustic manometer
US3214976A (en) Temperature measuring apparatus
US4495818A (en) Cylindrical vibrator type pressure transducer
Bean et al. Development of a primary standard for the measurement of dynamic pressure and temperature
GB1219231A (en) Apparatus and method for measuring the velocity of flow of a fluid
US3885436A (en) Temperature detecting system
US2927301A (en) Measurement of liquid levels in wells
US3427881A (en) System for measuring temperature
US3521492A (en) Fast response pressure gage
US3343403A (en) Apparatus for the measurement of the velocity of sound in a gas
US4194385A (en) Densitometer calibration method
US3144767A (en) Method and apparatus for determining fluid flow rate
US2936612A (en) Avoidance of fatigue effects under dynamic strain
Wente et al. A high efficiency receiver for a horn-type loud speaker of large power capacity
US3089341A (en) Quick-response temperature-corrected internal-type pressure gage
US3148536A (en) Ultrasonic thickness gage

Legal Events

Date Code Title Description
AS Assignment

Owner name: ITT CORPORATION

Free format text: CHANGE OF NAME;ASSIGNOR:INTERNATIONAL TELEPHONE AND TELEGRAPH CORPORATION;REEL/FRAME:004389/0606

Effective date: 19831122